Grid transparency and grid hole pattern control for ion beam uniformity

ABSTRACT

A design process for varying hole locations or sizes or both in an ion beam grid includes identifying a control grid to be modified; obtaining a change factor for the grid pattern; and using the change factor to generate a new grid pattern. The change factor is one or both of a hole location change factor or a hole diameter change factor. Also included is an ion beam grid having the characteristic of hole locations or sizes or both defined by a change factor modification of control grid hole locations or sizes or both.

RELATED APPLICATIONS

This application claims benefit of U.S. Provisional Application No. 60/677,386, entitled “GRID TRANSPARENCY AND GRID HOLE PATTERN CONTROL FOR ION BEAM UNIFORMITY” and filed Mar. 31, 2005, specifically incorporated by reference herein for all that it discloses or teaches. The present application is also a continuation of U.S. patent application Ser. No. 11/395,354, entitled “GRID TRANSPARENCY AND GRID HOLE PATTERN CONTROL FOR ION BEAM UNIFORMITY” and filed Mar. 31, 2006, specifically incorporated by reference herein for all that it discloses or teaches.

TECHNICAL FIELD

The described subject matter relates to a technique of ion source grid hole pattern design and control of grid transparency using stretching and/or shrinking of distances between grid holes, typically radially or linearly, where the grids are typically the electrodes of a broad beam ion acceleration system.

BACKGROUND

One of the issues in the development and usage of broad beam ion sources is in the production of very uniform ion beam density profiles. Since electric discharge plasmas do not themselves have a uniform distribution of ion density, ion sources which utilize ions generated in the plasma typically have non-uniform ion beam density profiles. Though the discussion here references beam grids, for example for ion sources, it applies generally to any charged particle broad beam source including both positive and negative ion beam sources and electron sources.

In order to solve this problem and achieve higher uniformities of ion beam current densities, ion extraction grids of gridded ion sources have been developed with variations of grid open area fraction (grid transparency) over the entire grid pattern. Indeed many have discrete sections of grid patterns in each of which may be different hole-to-hole distances and/or different hole diameters. Such ion extraction grids have been provided as solutions for various applications. At higher requirements of ion beam current density uniformities, however, the boundaries of such discrete sections may still cause unwanted disturbances in ion beam current density uniformities.

FIG. 1 shows one example of an arbitrary conventional grid pattern which has multiple discrete radially defined zones for grid transparency (the concentric circles being indicative of, and demarcating the boundaries between zones). Within each zone, the grid design is typically filled with repeating patterns to obtain a constant grid transparency within that zone. At the boundaries of zones, however, the transition between one zone and another may not be smooth, resulting in local discontinuities in the grid hole density, and, if left uncorrected, in the beam current density. FIG. 2 shows typical irregularities at both radial and azimuthal zone boundaries (note, the small black circles show locations of holes if they were equally spaced). These zone boundaries may be radial and various azimuthal boundaries may appear as shown here or, depending on the particular design, there may be other boundaries where either the hole size or spacing changes discontinuously. (Note, the six areas unpopulated with holes that are observed at the second radial boundary from the center in FIG. 1 are a result of other design features not relevant to the subject of this disclosure.) Conventionally, any adjustment to smooth the transition at the boundaries has been done by design personnel on a hole-by-hole basis. Shown in FIG. 3 is a distribution of grid transparency using an arbitrary unit as a function of radius in another arbitrary conventional grid design. The scattered data points in FIG. 3 are associated with boundaries where the patterns do not match and holes have been manually adjusted.

SUMMARY

Disclosed is a design process for varying hole locations or sizes in an ion beam grid including identifying a control grid to be modified; obtaining a hole location and/or hole size change factor for the grid pattern; and, using the change factor to generate a new grid pattern, which may also be referred to as “scaling” the grid transparency. Further disclosed are grids generated using the described design patterns.

BRIEF DESCRIPTION OF THE DRAWINGS

In the drawings:

FIG. 1 is a schematic plan view of a conventional ion beam grid pattern;

FIG. 2 is an enlarged portion of the schematic grid pattern of FIG. 1;

FIG. 3 is a plot of the distribution of transparency of another conventional grid pattern;

FIG. 4 presents a pair of enlarged portions of a schematic grid pattern;

FIG. 5 presents a pair of enlarged portions of an alternative schematic grid pattern;

FIG. 6, which includes sub-part FIGS. 6A, 6B, 6C and 6D, is a collection of graphs illustrating a process hereof;

FIG. 7 is another schematic plan view of a conventional ion beam grid pattern;

FIG. 8 is a schematic plan view of an ion beam grid pattern generated hereby;

FIG. 9 is a plot of a radial plasma ion density profile which may be used herewith;

FIG. 10 is a flow chart depiction of a design process hereof; and,

FIG. 11 is another flow chart depiction of a design process hereof.

DETAILED DESCRIPTION

An objective design process for varying hole locations and the hole-to-hole distances therebetween in an ion beam grid has been developed using a mathematical model to change grid transparency, also known as grid open area fraction. The new technique or techniques hereof do not require discrete zones (such as those shown in FIGS. 1 and 2) and, therefore, may substantially eliminate tedious and subjective manipulation of moving grid holes at boundaries of the zones. Rather, this design process provides for substantially continuously varying by “stretching” and/or “shrinking” the hole-to-hole distances to continuously or substantially continuously vary the grid ion transparency (open area) to compensate for plasma non-uniformities or beam non-uniformities due to other causes. In addition to the process, also thus developed are new grids manufactured with a substantially continuously varying transparency based on a design process hereof. The result of either or both will typically be greater control of ion beam uniformity. Though the discussion here references beam grids, for example for ion sources, it applies generally to any charged particle broad beam source including either positive or negative ion beam sources or electron sources.

This mathematically based process for developing grid transparencies may solve the shortcomings of current grid pattern design techniques, which use discrete sections or zones of established hole-to-hole distances or hole diameters, by instead using a substantially smooth, substantially continuous variation of hole-to-hole distances or substantially continuously changing grid hole diameters. Exemplar design procedures according hereto are thus described in the following procedures.

A first general technique starts with an initial (original or control) grid pattern to be modified. Then, in a first alternative implementation, as shown in FIG. 4, radial coordinates of the initial pattern hole locations may be changed from r to R. However, when doing so, there should be the same number of grid holes in the range of (r−dr/2, r+dr/2) in the original pattern and in the range of (R−dR/2, R+dR/2) in the modified pattern. Assuming the grid transparency of the original and modified grid patterns may be given as functions of radius as f(r) and F(R), respectively,

${{{f(r)}2}\pi \; {r{dr}}} = {{{{{F(R)}2}\pi \; {R{dR}}}\therefore\frac{R}{r}} = {\frac{r{f(r)}}{R{F(R)}}.}}$

By solving this differential equation for the grid hole location change factor R(r) with a boundary condition of R(r=r₀)=r₀, a new grid pattern can be obtained which achieves a desired or desirable grid transparency profile F(R). Hereafter, the grid hole location change factor may alternatively be referred to as a location change factor or simply as a change factor.

In an alternative second implementation, the technique may also start with an initial (original or control) grid pattern to be modified. Then, as shown in FIG. 5, one of the Cartesian coordinates of each of several initial pattern hole locations may be changed from x to X, and as before, there should be the same number of grid holes in the range of (x−dx/2, x+dx/2) in the original pattern and in the range of (X−dX/2, X+dX/2) in the modified pattern. Assuming the grid transparency of the original and modified grid patterns are given as functions of Cartesian distance as h(x) and H(X), respectively,

${{h(x)}{dx}} = {{{{H(X)}{dX}}\therefore\frac{X}{x}} = {\frac{h(x)}{H(X)}.}}$

Then, by solving this differential equation for a location change factor X(x) with a arbitrary boundary condition (such as X(x)=0), a new grid pattern can be obtained, which achieves the desired grid transparency profile H(X). An example of an application of the general process hereof is described in relation to and shown in FIG. 10 (see description below) in flow chart form for both radial and linear pattern modifications. Though not described in detail here, a similar process could be used for azimuthal pattern modifications, where ⊖ is the azimuthal coordinate in a polar coordinate system and a comparable differential equation is solved for a location change factor ⊖(θ) with appropriate boundary conditions.

Various means may be used in solving differential equations such as these, as for example, may be found in commercially available software products such as MathCad or Mathematica. As another example, Microsoft Excel files have also been used for this purpose. A fourth (4^(th)) order Runge-Kutta routine is one example that may be used for solution of the differential equation, among other forward-marching techniques of any orders (such as the so-called Euler method if it is 1st order, e.g.). For the radial method, by providing f(r) and F(R), the user would then be able to obtain a location change factor R(r), which is used to radially move the grid hole locations from the original design position to obtain the modified hole pattern. Similarly, by providing h(x) and H(X), the user would then be able to obtain a location change factor X(x), which is used to linearly move the grid hole locations from the original design position to obtain the modified hole pattern for linear stretching/shrinking in Cartesian coordinate systems. Similarly, by providing p(θ) and P(⊖), the user would then be able to obtain a location change factor ⊖(θ), which is used to azimuthally move the grid hole locations from the original design position to obtain the modified hole pattern in polar coordinate systems.

Viewed in a different light, a procedure hereof may be described as follows using a ratio of grid transparency modification as an approximation. Step 0: Defining a desired ratio of grid transparency by this modification (i(x) in a Cartesian system or g(r) in a 2D radial system) to achieve a better ion beam density uniformity profile. Such profiles can be determined based on experiments or other methods. This may first involve identifying a control grid which may be sought to be modified. Then, Step 1: Based on the desired modification, a grid transparency change ratio may be approximated by solving differential equations, which have different formats depending on the direction of modification. In a Cartesian system, it is

${\frac{x^{\prime}}{x} = \frac{1}{(x)}},$

where the grid transparency change ratio i(x)=H(x)/h(x) is an approximation to H(X)/h(x) and x′(x) yields an approximation of location change factor X(x). In a 2D radial system, it is

${\frac{r^{\prime}}{r} = \frac{r}{r^{\prime}{g(r)}}},$

where the grid transparency change ratio g(r)=F(r)/f(r) is an approximation to F(R)/f(r) and r′(r) yields an approximation of location change factor R(r). Next, Step 2: Applying the solution of the above differential equation to the control grid hole pattern, a new grid pattern is obtained. As an optional further step, Step 3: If ion beam density profiles obtained with the new grid pattern do not provide the preferred level of uniformity, then, the above steps 1-2 (either alternatively or in addition to steps 0-2) with adjustment of the desired modification in grid transparency may be iterated. A flow of iterative steps according hereto is shown in and described relative to FIG. 11 (see description below). Again, a similar process could be used for azimuthal pattern modification.

This can be depicted somewhat graphically as shown in the four parts of FIG. 6 using a radial example. The first graph of FIG. 6, namely FIG. 6A, shows a non-uniform ion beam density profile as such might appear to a substrate of an approximate ten inch width. Note the mirroring left to right (about a central vertical axis) as might be expected from a circular grid as shown for example in FIG. 1. Note also that as might be expected, the density generally declines near the far edges, although a higher than normalized density may occur near or nearer the center. In contrast, the preferred uniform normalized density should more preferably appear as a flat line such as that shown in the third graph of FIG. 6, namely, FIG. 6C. Thus, the first step as set forth herein is to identify the grid wanting an improvement toward uniformity. The grid which produced the profile of FIG. 6A may be just such a grid. Then, the next step is to calculate the desired grid transparency change ratio. This change ratio is approximated by calculating a ratio between the desired and actual normalized beam current density at each radial position. The second plot of FIG. 6, namely, FIG. 6B, presents a graphical representation of such a grid transparency change ratio for the right half of the FIG. 6A graphical profile. Note, the top to bottom horizontal mirror image effect of the FIG. 6B plot relative to the right side portion of the FIG. 6A graph. Conceptually, the grid transparency change ratio plot of FIG. 6B may also represent an inverse relationship to the values of the initial values of the FIG. 6A graph. As such, the product of the initial values with the inverse values would approach if not equal the normalized value of the FIG. 6C graph. The differential equation solution r′(r) for this radial example is shown graphically as a difference of r′(r) from r in FIG. 6D. It represents a continuously varying location change factor that can be applied to the radial location of each hole in the original design to provide a new design, which will have improved uniformity performance approaching the ideal shown in FIG. 6C. Note that, while the holes at the edge move significantly (up to in this particular example about 2mm), adjacent holes also move a similar amount so that the distance between adjacent holes changes only slightly. Therefore, in the example discussed above, the radial location of every hole in the original discrete zoned pattern was moved, i.e., “stretched/shrunk,” in a manner such that the new hole-to-hole spacing continuously or substantially continuously varied from the original spacing, resulting in a new pattern that, though perhaps still containing discrete zones, may better satisfy the improved uniformity criteria.

In addition to using the technique for improving the performance of an initial discrete zoned pattern, the technique can also be used for design of a new pattern with continuously varying hole spacing. In one of the examples for this case, a continuously varying grid transparency change ratio g(r) or i(x) may be used to approximate a discrete zoned design and input to the differential equation. The resulting location change factor solution r′(r) (approximation of R(r)) or x′(x) (approximation of X(x)) may functionally duplicate yet “smooth” the original discrete zoned design. A sample of such a discrete zoned pattern is shown in FIG. 7. In FIG. 7, the irregularity of the hole pattern can easily be seen in areas extending radially outwardly from the six areas of absent holes. By application of the process described here, a smooth, continuously varying adjustment of grid hole locations can then provide the smooth pattern of the grid as shown for example in FIG. 8. The result may then be greater control of ion beam uniformity because the discontinuities associated with the discrete zones may thus have been eliminated.

Thus, a mathematical model was developed to continuously or substantially continuously scale a grid pattern design to achieve a desired improved ion beam uniformity. A few grid sets were designed using this model and etch rate measurements showed improvement of ion beam uniformity when they were used in ion beam etch applications. The technique has been applied to ion source grid design, and tests indicate predictable improvement of grid performance in terms of ion beam current density uniformity, and improved etch rate distributions. Note that in some cases the initial designs were discrete zoned control designs which were “stretched” continuously to compensate for non-uniformities found in experimentally measured etch profiles. Moreover, this design process has been iterated in series with a ray-tracing model to provide a continuously varying transparency design. This iteration process was used to functionally duplicate yet “smooth” the original discrete zoned design. The intent may thus be to provide a continuously varying transparency design without any discrete zones but that would functionally duplicate the original discrete zoned design as closely as possible with still greater etch uniformity. This continuously varying baseline design may then serve as a starting point for further experimentally based iterations to optimize grid performance at specific operating conditions relevant to a particular application.

It has thus been found that in general, continuously or substantially continuously varying transparency designs may be desirable. Given a measured plasma density radial profile or a radial beam current density as a starting point, this technique is capable of providing such designs.

Yet another implementation of varying grid transparency designs using change factors such as described herein may be to substantially continuously change hole diameters. A process for establishing a design with substantially continuously varying hole diameters may be implemented in the following manner. When an original grid design having hole diameters, d, as a function of their radial coordinates, r, as d(r), is established and a desired modified grid design of a desired grid transparency with a grid transparency change ratio j(r) is known; then, a modified grid design should have hole diameters of:

d′(r)=d(r)×√{square root over (j(r))}

where d′(r) is a new diameter, which is designated hereafter as a hole diameter change factor or, alternatively, may simply be referred to as a change factor. Alternatively, if the hole diameters and desired grid transparency change ratio are given in a Cartesian system as d(x) and k(x), respectively, then the modified grid design diameters would be shown by:

d′(x)=d(x)×√{square root over (k(x))}

where d′(x) is a new diameter, which is also designated hereafter as a hole diameter change factor or simply as a change factor.

Moreover, techniques of varying hole positions and hole diameters may feasibly be combined together. An overall desired grid transparency change ratio, l(x) or m(r), can be achieved by combining a desired grid transparency change ratio, k(x) or j(r), which may be achieved by varying hole diameters and a different desired grid transparency change ratio, i(x) or g(r), which may be achieved by varying hole locations where:

l(x)=i(x)×k(x),

or

m(r)=g(r)×j(r).

For each overall change ratio, l(x) or m(r), a designer may arbitrarily partition grid transparency change ratios (i(x) and k(x), or g(r) and j(r)) as long as the above equations are satisfied. Then, each grid transparency change ratio can be used to solve for a location change factor, x′(x) or r′(r), and a diameter change factor, d′(x) or d′(r).

While the various implementations described above used as a starting point an original or control grid pattern together with the corresponding measured beam current density profile from the extracted beam to determine a grid transparency change ratio for a new grid, it is also possible to start with either a measured or a theoretically modeled plasma ion density profile. This could be useful for designing the first iteration grids for a new device based on either a theoretical model for the discharge or measurements of ion plasma density in a prototype chamber. Here the distinction is made between the plasma ion density profile associated with the ion source that supplies ions to the grid system and the density profile of the ion beam extracted by the grids from that source. An example of such a radial ion density profile is shown in FIG. 9. In this case, one might begin the process using as a control grid pattern one with a constant hole spacing and use as f(r) the function representing the plasma ion density profile or any other initial starting point.

A further detailed process herefor may be as follows, and as shown in FIG. 10. In particular, a first step may generally involve the establishment of a control grid pattern whether of a previously calculated or previously manufactured grid, which grid transparency is given as f(r) or h(x). Then, after the designer specifies a new grid transparency F(R) or H(X), the grid hole location change factor may be obtained by solving one or more differential equations. An example of solving the differential equation(s) may include a usage of a 4th order Runge Kutta method. For example, when a radial differential equation of

$\frac{R}{r} = \frac{r{f(r)}}{R{F(R)}}$

is solved with this method where locations and boundary conditions (r_(n) (n=0,1,2, . . . ) and R₀=r₀) are defined, inter alia (for example, various design constraints such as grid pattern overall size and/or minimum thickness between holes), R_(n+1) would be obtained using r_(n), R_(n), f(r), F(R), and Δr(=r_(n+1)−r_(n)) according to the following equations:

${k_{1} = {\Delta \; {r\frac{r_{n}{f\left( r_{n} \right)}}{R_{n}{F\left( R_{n} \right)}}}}},{k_{2} = {\Delta \; {r\frac{\left( {r_{n} + \frac{\Delta \; r}{2}} \right){f\left( {r_{n} + \frac{\Delta \; r}{2}} \right)}}{\left( {R_{n} + \frac{k_{1}}{2}} \right){F\left( {R_{n} + \frac{k_{1}}{2}} \right)}}}}},{k_{3} = {\Delta \; {r\frac{\left( {r_{n} + \frac{\Delta \; r}{2}} \right){f\left( {r_{n} + \frac{\Delta \; r}{2}} \right)}}{\left( {R_{n} + \frac{k_{2}}{2}} \right){F\left( {R_{n} + \frac{k_{2}}{2}} \right)}}}}},{k_{4} = {\Delta \; {r\frac{\left( {r_{n} + {\Delta \; r}} \right){f\left( {r_{n} + {\Delta \; r}} \right)}}{\left( {R_{n} + k_{3}} \right){F\left( {R_{n} + k_{3}} \right)}}}}},{R_{n + 1} = {R_{n} + {\frac{k_{1} + {k_{2}2} + {k_{3}2} + k_{4}}{6}.}}}$

The solution to the differential equation may then give the new location for the hole as a grid hole location change factor in the form of arrays of r_(n) and R_(n). Note, tables or other utilities may be used for developing and/or tracking the modified locations relative to the original locations. This method can be used for radial and/or linear coordinate systems as indicated in FIG. 10.

The alternate implementation shown in FIG. 11 start with approximated grid transparency change ratio, g(r) or i(x). In this implementation example, the initial operation or Step 0, may involve defining a desired ratio of grid transparencies as g(r) (which may be obtained as F(R=r)/f(r)) or i(x) (which may be obtained as H(X=x)/h(x)). Such an example is shown in FIG. 6B. Then, in a further operation, here, Step 1, a combination of a definition and calculation with a subsequent determination may be performed. First, this may involve a defining of r_(n) or x_(n) (n=0,1,2, . . . ) with a setting of r′₀=r₀ or x′₀=x₀ and solving one or both of the following differential equations:

${\frac{r^{\prime}}{r} = \frac{r}{R{g(r)}}},{or}$ $\frac{x^{\prime}}{x} = \frac{1}{(x)}$

which gives a grid hole location change factor in the form of arrays of r_(n) and r′_(n) or that of x_(n) and x′_(n). Then, proceeding to Step 2, a grid may be manufactured with a hole pattern based on the relations of r_(n) and r′_(n) or of x_(n) and x′_(n). After this Step 2, then a further determination of whether the new design yields a desired grid transparency can be made, where if so the process of FIG. 11 is complete. However, if not, then an iteration of both Steps 1 and 2 may be re-done. If necessary, a modification of a desired grid transparency change ratio, g(r) or i(x), based on a grid transparency may be obtained relative to and/or from a previous iteration.

Though many of the examples above mention ion beam grids and ion beam sources, the design processes and grids manufactured based thereon could apply generally to any charged particle broad beam source including either positive or negative ion beam sources or electron sources. In such cases, the spatial functions of interest would be for example those such as the upstream negative ion density (and/or arrival rate) profiles or electron density (and/or arrival rate) profiles and the corresponding downstream charged particle beam current density profiles, where upstream and downstream are defined relative to the extraction grid. Likewise, though various forms of electrical discharge sources, for example DC or RF excited discharges, are common as plasma sources for ion beam extraction, the design processes described here and the grids manufactured thereon are expected to be generally applicable to charged particle beams extracted from plasmas generated by any one of numerous alternate means, for example, microwave plasmas, standing wave sheet plasmas, laser stimulated plasmas, surface contact or emission plasmas, and from various non-plasma, single charge species field and surface emission devices, inter alia.

The above specification, examples and data provide a description of the process and structure and use of exemplary embodiments of the invention. However, other implementations are also contemplated within the scope of the present invention, including without limitation methods of providing and/or grids having holes of different shapes, sizes, and locations than those shown and/or described. In addition, while the description has described exemplary process and grids, other processes and grids may be employed within the scope of the invention. Since many implementations can be made and/or used without departing from the spirit and scope of the invention, the invention resides in the claims hereinafter appended. 

1. A beam grid comprising: a modified pattern of holes with a region having a grid hole density that continuously varies with distance from a reference on the beam grid and a constant grid hole size, wherein the modified pattern of holes is derived from an initial pattern of holes.
 2. The beam grid of claim 1, wherein the modified pattern of holes is derived from the initial pattern of holes using a change factor.
 3. The beam grid of claim 1, wherein the reference is a point.
 4. The beam grid of claim 1, wherein the reference is a line.
 5. The beam grid of claim 1, wherein the reference is at a center of the beam grid.
 6. The beam grid of claim 1, wherein the beam grid is generally circular.
 7. The beam grid of claim 1, wherein the region having a continuously varying grid hole density includes all of the modified pattern of holes.
 8. The beam grid of claim 1, wherein the modified pattern of holes has no discrete regions with different hole densities.
 9. The beam grid of claim 1, further comprising: a mounting pattern of holes arranged about a perimeter of the beam grid for mounting the beam grid to an ion source.
 10. A beam grid comprising: a modified pattern of holes with region having a grid hole density and grid hole size that continuously varies with distance from a reference on the beam grid, wherein the modified pattern of holes is derived from an initial pattern of holes.
 11. The beam grid of claim 10, wherein the modified pattern of holes is derived from the initial pattern of holes using a change factor.
 12. The beam grid of claim 10, wherein the reference is a point.
 13. The beam grid of claim 10, wherein the reference is a line.
 14. The beam grid of claim 10, wherein the reference is a center of the beam grid.
 15. The beam grid of claim 10, wherein the beam grid is generally circular.
 16. The beam grid of claim 10, wherein the region having a continuously varying grid hole density and grid hole size includes all of the modified pattern of holes.
 17. The beam grid of claim 10, wherein the modified pattern of holes has no discrete regions with different hole sizes.
 18. The beam grid of claim 10, wherein the modified pattern of holes has no discrete regions with different hole densities.
 19. The beam grid of claim 10, further comprising: a mounting pattern of holes arranged about a perimeter of the beam grid for mounting the beam grid to an ion source. 